ar X iv : h ep - p h / 92 06 26 5 v 2 1 8 A ug 1 99 2 June 26 , 1992 LBL - 32531 Global Quantization in Gauge Orbit

We generalize our discussions and give more general physical applications of a new solution to the strong CP problem with magnetic monopoles as originally proposed by the author. Especially, we will discuss about the global topological structure in the relevant gauge orbit spaces to be clarified. As it is shown that in non-abelian gauge theories with a θ term, the induced gauge orbit space with gauge potentials and gauge functions restricted on the space boundary S has a magnetic monopole structure and the gauge orbit space has a vortex structure if there is a magnetic monopole in the ordinary space. The Dirac’s quantization conditions in the quantum theories ensure that the vacuum angle θ in the gauge theories must be quantized. The quantization rule is given by θ = 2π/n (n 6= 0) with n being the topological charge of the magnetic monopole. Therefore, the strong CP problem is automatically solved in the presence of a magnetic monopole of charge ±1 with θ = ±2π, or magnetic monopoles of very large total topological charge (|n| ≥ 102π) if it is consistent with the abundance of magnetic monopoles. Where in the first case with a magnetic monopole of topological charge 1 or -1, we mean the strong CPviolation can be only very small by the measurements implemented so far. Since θ = ±2π correspond to different monopole sectors, the CP can not be conserved exactly in strong interactions in this case. In the second case, the strong CP cannot be conserved either for large but finite n. The fact that the strong CP-violation measured so far can be only so small or vanishing may be a signal for the existence of magnetic monopoles. We also conjecture that the parity violation and CP violation in weak interaction fundamentally may intimately connected to the magnetic monopoles. The relevance to the UA(1) problem is also discussed. The existence of colored magnetic monopoles may also solve the UA(1) problem. In the presence of U(1) or monopoles as color singlets, the ’t Hooft’s solution to